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Pairwise Configurational Entropy

Abstract

Pairwise smoothing increases the entropy of independent Bernoulli coordinates conditional on their sum.

Theorem 1.1 (Continuity at the boundary).

Proof. Machine-checked in Lean as D5/S3/Entropy/PoissonBinomial/ConfigurationalEntropyStep.continuous_F (✓ std3). ∎

Source. Repository-derived.

Acknowledgement. D. Monkman; J. Sirker (2023). Symmetry-resolved entanglement: general considerations, calculation from correlation functions, and bounds for symmetry-protected topological phases. DOI: 10.48550/arXiv.2307.05820. URL: https://arxiv.org/abs/2307.05820.

Commentary.

Each Poisson-binomial mass is a finite sum of products of the Bernoulli parameters and their complements. Continuity of binary entropy and of negative x log x, including zero, therefore gives continuity of F on the whole parameter space.

Theorem 1.2 (An interior T-transform increases F).

Proof. Machine-checked in Lean as D5/S3/Entropy/PoissonBinomial/ConfigurationalEntropyStep.F_le_interiorT (✓ std3). ∎

Source. Repository-derived.

Acknowledgement. D. Monkman; J. Sirker (2023). Symmetry-resolved entanglement: general considerations, calculation from correlation functions, and bounds for symmetry-protected topological phases. DOI: 10.48550/arXiv.2307.05820. URL: https://arxiv.org/abs/2307.05820.

Commentary.

For two distinct coordinates p at least q, move them to p-s and q+s. The other coordinates give a normalized Poisson-binomial law supported through M-2. Removing the pair expresses the full law as its three-point convolution.

At an interior pair p>q, write A=p(1−q) and B=q(1−p), so A−B=p−q. The derivative of F in the smoothing direction factors as (p−q)[(log A−log B)/(A−B)−d], where d is the entropy derivative of the three-point convolution in direction (1,−2,1). The binary part is controlled by the logarithmic bound A1; the convolution part satisfies d≤−log(AB).

The entropy-direction bound for the convolution and the logarithmic divided-difference bound show that the derivative of F is nonnegative up to the midpoint. At equal coordinates the derivative is zero. Coordinate permutation invariance handles steps beyond the midpoint. No strictness or equality characterization is asserted.

References